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34 * GROwing Monsters And Cloning Shrimps
41 #include<catamount/dclock.h>
47 #ifdef HAVE_SYS_TIME_H
60 #include "chargegroup.h"
82 #include "pull_rotation.h"
83 #include "gmx_random.h"
86 #include "gmx_wallcycle.h"
100 typedef struct gmx_timeprint {
105 /* Portable version of ctime_r implemented in src/gmxlib/string2.c, but we do not want it declared in public installed headers */
107 gmx_ctime_r(const time_t *clock,char *buf, int n);
113 #ifdef HAVE_GETTIMEOFDAY
117 gettimeofday(&t,NULL);
119 seconds = (double) t.tv_sec + 1e-6*(double)t.tv_usec;
125 seconds = time(NULL);
132 #define difftime(end,start) ((double)(end)-(double)(start))
134 void print_time(FILE *out,gmx_runtime_t *runtime,gmx_large_int_t step,
135 t_inputrec *ir, t_commrec *cr)
138 char timebuf[STRLEN];
142 #ifndef GMX_THREAD_MPI
148 fprintf(out,"step %s",gmx_step_str(step,buf));
149 if ((step >= ir->nstlist))
151 if ((ir->nstlist == 0) || ((step % ir->nstlist) == 0))
153 /* We have done a full cycle let's update time_per_step */
154 runtime->last = gmx_gettime();
155 dt = difftime(runtime->last,runtime->real);
156 runtime->time_per_step = dt/(step - ir->init_step + 1);
158 dt = (ir->nsteps + ir->init_step - step)*runtime->time_per_step;
164 finish = (time_t) (runtime->last + dt);
165 gmx_ctime_r(&finish,timebuf,STRLEN);
166 sprintf(buf,"%s",timebuf);
167 buf[strlen(buf)-1]='\0';
168 fprintf(out,", will finish %s",buf);
171 fprintf(out,", remaining runtime: %5d s ",(int)dt);
175 fprintf(out," performance: %.1f ns/day ",
176 ir->delta_t/1000*24*60*60/runtime->time_per_step);
179 #ifndef GMX_THREAD_MPI
193 static double set_proctime(gmx_runtime_t *runtime)
199 prev = runtime->proc;
200 runtime->proc = dclock();
202 diff = runtime->proc - prev;
206 prev = runtime->proc;
207 runtime->proc = clock();
209 diff = (double)(runtime->proc - prev)/(double)CLOCKS_PER_SEC;
213 /* The counter has probably looped, ignore this data */
220 void runtime_start(gmx_runtime_t *runtime)
222 runtime->real = gmx_gettime();
224 set_proctime(runtime);
225 runtime->realtime = 0;
226 runtime->proctime = 0;
228 runtime->time_per_step = 0;
231 void runtime_end(gmx_runtime_t *runtime)
237 runtime->proctime += set_proctime(runtime);
238 runtime->realtime = now - runtime->real;
242 void runtime_upd_proc(gmx_runtime_t *runtime)
244 runtime->proctime += set_proctime(runtime);
247 void print_date_and_time(FILE *fplog,int nodeid,const char *title,
248 const gmx_runtime_t *runtime)
251 char timebuf[STRLEN];
252 char time_string[STRLEN];
259 tmptime = (time_t) runtime->real;
260 gmx_ctime_r(&tmptime,timebuf,STRLEN);
264 tmptime = (time_t) gmx_gettime();
265 gmx_ctime_r(&tmptime,timebuf,STRLEN);
267 for(i=0; timebuf[i]>=' '; i++)
269 time_string[i]=timebuf[i];
273 fprintf(fplog,"%s on node %d %s\n",title,nodeid,time_string);
277 static void sum_forces(int start,int end,rvec f[],rvec flr[])
282 pr_rvecs(debug,0,"fsr",f+start,end-start);
283 pr_rvecs(debug,0,"flr",flr+start,end-start);
285 for(i=start; (i<end); i++)
286 rvec_inc(f[i],flr[i]);
290 * calc_f_el calculates forces due to an electric field.
292 * force is kJ mol^-1 nm^-1 = e * kJ mol^-1 nm^-1 / e
294 * Et[] contains the parameters for the time dependent
295 * part of the field (not yet used).
296 * Ex[] contains the parameters for
297 * the spatial dependent part of the field. You can have cool periodic
298 * fields in principle, but only a constant field is supported
300 * The function should return the energy due to the electric field
301 * (if any) but for now returns 0.
304 * There can be problems with the virial.
305 * Since the field is not self-consistent this is unavoidable.
306 * For neutral molecules the virial is correct within this approximation.
307 * For neutral systems with many charged molecules the error is small.
308 * But for systems with a net charge or a few charged molecules
309 * the error can be significant when the field is high.
310 * Solution: implement a self-consitent electric field into PME.
312 static void calc_f_el(FILE *fp,int start,int homenr,
313 real charge[],rvec x[],rvec f[],
314 t_cosines Ex[],t_cosines Et[],double t)
320 for(m=0; (m<DIM); m++)
327 Ext[m] = cos(Et[m].a[0]*(t-t0))*exp(-sqr(t-t0)/(2.0*sqr(Et[m].a[2])));
331 Ext[m] = cos(Et[m].a[0]*t);
340 /* Convert the field strength from V/nm to MD-units */
341 Ext[m] *= Ex[m].a[0]*FIELDFAC;
342 for(i=start; (i<start+homenr); i++)
343 f[i][m] += charge[i]*Ext[m];
352 fprintf(fp,"%10g %10g %10g %10g #FIELD\n",t,
353 Ext[XX]/FIELDFAC,Ext[YY]/FIELDFAC,Ext[ZZ]/FIELDFAC);
357 static void calc_virial(FILE *fplog,int start,int homenr,rvec x[],rvec f[],
358 tensor vir_part,t_graph *graph,matrix box,
359 t_nrnb *nrnb,const t_forcerec *fr,int ePBC)
364 /* The short-range virial from surrounding boxes */
366 calc_vir(fplog,SHIFTS,fr->shift_vec,fr->fshift,vir_part,ePBC==epbcSCREW,box);
367 inc_nrnb(nrnb,eNR_VIRIAL,SHIFTS);
369 /* Calculate partial virial, for local atoms only, based on short range.
370 * Total virial is computed in global_stat, called from do_md
372 f_calc_vir(fplog,start,start+homenr,x,f,vir_part,graph,box);
373 inc_nrnb(nrnb,eNR_VIRIAL,homenr);
375 /* Add position restraint contribution */
376 for(i=0; i<DIM; i++) {
377 vir_part[i][i] += fr->vir_diag_posres[i];
380 /* Add wall contribution */
381 for(i=0; i<DIM; i++) {
382 vir_part[i][ZZ] += fr->vir_wall_z[i];
386 pr_rvecs(debug,0,"vir_part",vir_part,DIM);
389 static void print_large_forces(FILE *fp,t_mdatoms *md,t_commrec *cr,
390 gmx_large_int_t step,real pforce,rvec *x,rvec *f)
394 char buf[STEPSTRSIZE];
397 for(i=md->start; i<md->start+md->homenr; i++) {
399 /* We also catch NAN, if the compiler does not optimize this away. */
400 if (fn2 >= pf2 || fn2 != fn2) {
401 fprintf(fp,"step %s atom %6d x %8.3f %8.3f %8.3f force %12.5e\n",
402 gmx_step_str(step,buf),
403 ddglatnr(cr->dd,i),x[i][XX],x[i][YY],x[i][ZZ],sqrt(fn2));
408 void do_force(FILE *fplog,t_commrec *cr,
409 t_inputrec *inputrec,
410 gmx_large_int_t step,t_nrnb *nrnb,gmx_wallcycle_t wcycle,
413 gmx_groups_t *groups,
414 matrix box,rvec x[],history_t *hist,
418 gmx_enerdata_t *enerd,t_fcdata *fcd,
419 real *lambda,t_graph *graph,
420 t_forcerec *fr,gmx_vsite_t *vsite,rvec mu_tot,
421 double t,FILE *field,gmx_edsam_t ed,
428 gmx_bool bSepDVDL,bStateChanged,bNS,bFillGrid,bCalcCGCM,bBS;
429 gmx_bool bDoLongRange,bDoForces,bSepLRF;
430 gmx_bool bDoAdressWF;
432 real e,v,dvdlambda[efptNR];
433 real dvdl_dum,lambda_dum;
435 float cycles_ppdpme,cycles_pme,cycles_seppme,cycles_force;
437 start = mdatoms->start;
438 homenr = mdatoms->homenr;
440 bSepDVDL = (fr->bSepDVDL && do_per_step(step,inputrec->nstlog));
442 clear_mat(vir_force);
446 pd_cg_range(cr,&cg0,&cg1);
451 if (DOMAINDECOMP(cr))
453 cg1 = cr->dd->ncg_tot;
465 bStateChanged = (flags & GMX_FORCE_STATECHANGED);
466 bNS = (flags & GMX_FORCE_NS) && (fr->bAllvsAll==FALSE);
467 bFillGrid = (bNS && bStateChanged);
468 bCalcCGCM = (bFillGrid && !DOMAINDECOMP(cr));
469 bDoLongRange = (fr->bTwinRange && bNS && (flags & GMX_FORCE_DOLR));
470 bDoForces = (flags & GMX_FORCE_FORCES);
471 bSepLRF = (bDoLongRange && bDoForces && (flags & GMX_FORCE_SEPLRF));
472 /* should probably move this to the forcerec since it doesn't change */
473 bDoAdressWF = ((fr->adress_type!=eAdressOff));
477 update_forcerec(fplog,fr,box);
479 /* Calculate total (local) dipole moment in a temporary common array.
480 * This makes it possible to sum them over nodes faster.
482 calc_mu(start,homenr,
483 x,mdatoms->chargeA,mdatoms->chargeB,mdatoms->nChargePerturbed,
487 if (fr->ePBC != epbcNONE) {
488 /* Compute shift vectors every step,
489 * because of pressure coupling or box deformation!
491 if ((flags & GMX_FORCE_DYNAMICBOX) && bStateChanged)
492 calc_shifts(box,fr->shift_vec);
495 put_charge_groups_in_box(fplog,cg0,cg1,fr->ePBC,box,
496 &(top->cgs),x,fr->cg_cm);
497 inc_nrnb(nrnb,eNR_CGCM,homenr);
498 inc_nrnb(nrnb,eNR_RESETX,cg1-cg0);
500 else if (EI_ENERGY_MINIMIZATION(inputrec->eI) && graph) {
501 unshift_self(graph,box,x);
504 else if (bCalcCGCM) {
505 calc_cgcm(fplog,cg0,cg1,&(top->cgs),x,fr->cg_cm);
506 inc_nrnb(nrnb,eNR_CGCM,homenr);
511 move_cgcm(fplog,cr,fr->cg_cm);
514 pr_rvecs(debug,0,"cgcm",fr->cg_cm,top->cgs.nr);
518 if (!(cr->duty & DUTY_PME)) {
519 /* Send particle coordinates to the pme nodes.
520 * Since this is only implemented for domain decomposition
521 * and domain decomposition does not use the graph,
522 * we do not need to worry about shifting.
525 wallcycle_start(wcycle,ewcPP_PMESENDX);
527 bBS = (inputrec->nwall == 2);
530 svmul(inputrec->wall_ewald_zfac,boxs[ZZ],boxs[ZZ]);
533 gmx_pme_send_x(cr,bBS ? boxs : box,x,
534 mdatoms->nChargePerturbed,lambda[efptCOUL],
535 ( flags & GMX_FORCE_VIRIAL),step);
537 wallcycle_stop(wcycle,ewcPP_PMESENDX);
541 /* Communicate coordinates and sum dipole if necessary */
544 wallcycle_start(wcycle,ewcMOVEX);
545 if (DOMAINDECOMP(cr))
547 dd_move_x(cr->dd,box,x);
551 move_x(fplog,cr,GMX_LEFT,GMX_RIGHT,x,nrnb);
553 /* When we don't need the total dipole we sum it in global_stat */
554 if (bStateChanged && NEED_MUTOT(*inputrec))
556 gmx_sumd(2*DIM,mu,cr);
558 wallcycle_stop(wcycle,ewcMOVEX);
563 /* update adress weight beforehand */
566 /* need pbc for adress weight calculation with pbc_dx */
567 set_pbc(&pbc,inputrec->ePBC,box);
568 if(fr->adress_site == eAdressSITEcog)
570 update_adress_weights_cog(top->idef.iparams,top->idef.il,x,fr,mdatoms,
571 inputrec->ePBC==epbcNONE ? NULL : &pbc);
573 else if (fr->adress_site == eAdressSITEcom)
575 update_adress_weights_com(fplog,cg0,cg1,&(top->cgs),x,fr,mdatoms,
576 inputrec->ePBC==epbcNONE ? NULL : &pbc);
578 else if (fr->adress_site == eAdressSITEatomatom){
579 update_adress_weights_atom_per_atom(cg0,cg1,&(top->cgs),x,fr,mdatoms,
580 inputrec->ePBC==epbcNONE ? NULL : &pbc);
584 update_adress_weights_atom(cg0,cg1,&(top->cgs),x,fr,mdatoms,
585 inputrec->ePBC==epbcNONE ? NULL : &pbc);
593 fr->mu_tot[i][j] = mu[i*DIM + j];
597 if (fr->efep == efepNO)
599 copy_rvec(fr->mu_tot[0],mu_tot);
606 (1.0 - lambda[efptCOUL])*fr->mu_tot[0][j] + lambda[efptCOUL]*fr->mu_tot[1][j];
611 reset_enerdata(&(inputrec->opts),fr,bNS,enerd,MASTER(cr));
612 clear_rvecs(SHIFTS,fr->fshift);
616 wallcycle_start(wcycle,ewcNS);
618 if (graph && bStateChanged)
620 /* Calculate intramolecular shift vectors to make molecules whole */
621 mk_mshift(fplog,graph,fr->ePBC,box,x);
624 /* Reset long range forces if necessary */
627 /* Reset the (long-range) forces if necessary */
628 clear_rvecs(fr->natoms_force_constr,bSepLRF ? fr->f_twin : f);
631 /* Do the actual neighbour searching and if twin range electrostatics
632 * also do the calculation of long range forces and energies.
634 for (i=0;i<efptNR;i++) {dvdlambda[i] = 0;}
636 groups,&(inputrec->opts),top,mdatoms,
637 cr,nrnb,lambda,dvdlambda,&enerd->grpp,bFillGrid,
638 bDoLongRange,bDoForces,bSepLRF ? fr->f_twin : f);
641 fprintf(fplog,sepdvdlformat,"LR non-bonded",0.0,dvdlambda);
643 enerd->dvdl_lin[efptVDW] += dvdlambda[efptVDW];
644 enerd->dvdl_lin[efptCOUL] += dvdlambda[efptCOUL];
646 wallcycle_stop(wcycle,ewcNS);
649 if (inputrec->implicit_solvent && bNS)
651 make_gb_nblist(cr,inputrec->gb_algorithm,inputrec->rlist,
652 x,box,fr,&top->idef,graph,fr->born);
655 if (DOMAINDECOMP(cr))
657 if (!(cr->duty & DUTY_PME))
659 wallcycle_start(wcycle,ewcPPDURINGPME);
660 dd_force_flop_start(cr->dd,nrnb);
666 /* Enforced rotation has its own cycle counter that starts after the collective
667 * coordinates have been communicated. It is added to ddCyclF to allow
668 * for proper load-balancing */
669 wallcycle_start(wcycle,ewcROT);
670 do_rotation(cr,inputrec,box,x,t,step,wcycle,bNS);
671 wallcycle_stop(wcycle,ewcROT);
674 /* Start the force cycle counter.
675 * This counter is stopped in do_forcelow_level.
676 * No parallel communication should occur while this counter is running,
677 * since that will interfere with the dynamic load balancing.
679 wallcycle_start(wcycle,ewcFORCE);
683 /* Reset forces for which the virial is calculated separately:
684 * PME/Ewald forces if necessary */
687 if (flags & GMX_FORCE_VIRIAL)
689 fr->f_novirsum = fr->f_novirsum_alloc;
692 clear_rvecs(fr->f_novirsum_n,fr->f_novirsum);
696 clear_rvecs(homenr,fr->f_novirsum+start);
701 /* We are not calculating the pressure so we do not need
702 * a separate array for forces that do not contribute
711 /* Add the long range forces to the short range forces */
712 for(i=0; i<fr->natoms_force_constr; i++)
714 copy_rvec(fr->f_twin[i],f[i]);
717 else if (!(fr->bTwinRange && bNS))
719 /* Clear the short-range forces */
720 clear_rvecs(fr->natoms_force_constr,f);
723 clear_rvec(fr->vir_diag_posres);
725 if (inputrec->ePull == epullCONSTRAINT)
727 clear_pull_forces(inputrec->pull);
730 /* update QMMMrec, if necessary */
733 update_QMMMrec(cr,fr,x,mdatoms,box,top);
736 if ((flags & GMX_FORCE_BONDED) && top->idef.il[F_POSRES].nr > 0)
738 /* Position restraints always require full pbc. Check if we already did it for Adress */
739 if(!(bStateChanged && bDoAdressWF))
741 set_pbc(&pbc,inputrec->ePBC,box);
743 v = posres(top->idef.il[F_POSRES].nr,top->idef.il[F_POSRES].iatoms,
744 top->idef.iparams_posres,
745 (const rvec*)x,fr->f_novirsum,fr->vir_diag_posres,
746 inputrec->ePBC==epbcNONE ? NULL : &pbc,lambda[efptRESTRAINT],&(dvdlambda[efptRESTRAINT]),
747 fr->rc_scaling,fr->ePBC,fr->posres_com,fr->posres_comB);
750 fprintf(fplog,sepdvdlformat,
751 interaction_function[F_POSRES].longname,v,dvdlambda);
753 enerd->term[F_POSRES] += v;
754 /* This linear lambda dependence assumption is only correct
755 * when only k depends on lambda,
756 * not when the reference position depends on lambda.
757 * grompp checks for this. (verify this is still the case?)
759 enerd->dvdl_nonlin[efptRESTRAINT] += dvdlambda[efptRESTRAINT]; /* if just the force constant changes, this is linear,
760 but we can't be sure w/o additional checking that is
761 hard to do at this level of code. Otherwise,
762 the dvdl is not differentiable */
763 inc_nrnb(nrnb,eNR_POSRES,top->idef.il[F_POSRES].nr/2);
764 if ((inputrec->fepvals->n_lambda > 0) && (flags & GMX_FORCE_DHDL))
766 for(i=0; i<enerd->n_lambda; i++)
768 lambda_dum = (i==0 ? lambda[efptRESTRAINT] : inputrec->fepvals->all_lambda[efptRESTRAINT][i-1]);
769 v = posres(top->idef.il[F_POSRES].nr,top->idef.il[F_POSRES].iatoms,
770 top->idef.iparams_posres,
771 (const rvec*)x,NULL,NULL,
772 inputrec->ePBC==epbcNONE ? NULL : &pbc,lambda_dum,&dvdl_dum,
773 fr->rc_scaling,fr->ePBC,fr->posres_com,fr->posres_comB);
774 enerd->enerpart_lambda[i] += v;
779 if ((flags & GMX_FORCE_BONDED) && top->idef.il[F_FBPOSRES].nr > 0)
781 /* Flat-bottomed position restraints always require full pbc */
782 if(!(bStateChanged && bDoAdressWF))
784 set_pbc(&pbc,inputrec->ePBC,box);
786 v = fbposres(top->idef.il[F_FBPOSRES].nr,top->idef.il[F_FBPOSRES].iatoms,
787 top->idef.iparams_fbposres,
788 (const rvec*)x,fr->f_novirsum,fr->vir_diag_posres,
789 inputrec->ePBC==epbcNONE ? NULL : &pbc,
790 fr->rc_scaling,fr->ePBC,fr->posres_com);
791 enerd->term[F_FBPOSRES] += v;
792 inc_nrnb(nrnb,eNR_FBPOSRES,top->idef.il[F_FBPOSRES].nr/2);
795 /* Compute the bonded and non-bonded energies and optionally forces */
796 do_force_lowlevel(fplog,step,fr,inputrec,&(top->idef),
797 cr,nrnb,wcycle,mdatoms,&(inputrec->opts),
798 x,hist,f,enerd,fcd,mtop,top,fr->born,
799 &(top->atomtypes),bBornRadii,box,
800 inputrec->fepvals,lambda,graph,&(top->excls),fr->mu_tot,
803 cycles_force = wallcycle_stop(wcycle,ewcFORCE);
807 do_flood(fplog,cr,x,f,ed,box,step,bNS);
810 if (DOMAINDECOMP(cr))
812 dd_force_flop_stop(cr->dd,nrnb);
815 dd_cycles_add(cr->dd,cycles_force-cycles_pme,ddCyclF);
821 if (IR_ELEC_FIELD(*inputrec))
823 /* Compute forces due to electric field */
824 calc_f_el(MASTER(cr) ? field : NULL,
825 start,homenr,mdatoms->chargeA,x,fr->f_novirsum,
826 inputrec->ex,inputrec->et,t);
829 if (bDoAdressWF && fr->adress_icor == eAdressICThermoForce)
831 /* Compute thermodynamic force in hybrid AdResS region */
832 adress_thermo_force(start,homenr,&(top->cgs),x,fr->f_novirsum,fr,mdatoms,
833 inputrec->ePBC==epbcNONE ? NULL : &pbc);
836 /* Communicate the forces */
839 wallcycle_start(wcycle,ewcMOVEF);
840 if (DOMAINDECOMP(cr))
842 dd_move_f(cr->dd,f,fr->fshift);
843 /* Do we need to communicate the separate force array
844 * for terms that do not contribute to the single sum virial?
845 * Position restraints and electric fields do not introduce
846 * inter-cg forces, only full electrostatics methods do.
847 * When we do not calculate the virial, fr->f_novirsum = f,
848 * so we have already communicated these forces.
850 if (EEL_FULL(fr->eeltype) && cr->dd->n_intercg_excl &&
851 (flags & GMX_FORCE_VIRIAL))
853 dd_move_f(cr->dd,fr->f_novirsum,NULL);
857 /* We should not update the shift forces here,
858 * since f_twin is already included in f.
860 dd_move_f(cr->dd,fr->f_twin,NULL);
865 pd_move_f(cr,f,nrnb);
868 pd_move_f(cr,fr->f_twin,nrnb);
871 wallcycle_stop(wcycle,ewcMOVEF);
874 /* If we have NoVirSum forces, but we do not calculate the virial,
875 * we sum fr->f_novirum=f later.
877 if (vsite && !(fr->bF_NoVirSum && !(flags & GMX_FORCE_VIRIAL)))
879 wallcycle_start(wcycle,ewcVSITESPREAD);
880 spread_vsite_f(fplog,vsite,x,f,fr->fshift,FALSE,NULL,nrnb,
881 &top->idef,fr->ePBC,fr->bMolPBC,graph,box,cr);
882 wallcycle_stop(wcycle,ewcVSITESPREAD);
886 wallcycle_start(wcycle,ewcVSITESPREAD);
887 spread_vsite_f(fplog,vsite,x,fr->f_twin,NULL,FALSE,NULL,
889 &top->idef,fr->ePBC,fr->bMolPBC,graph,box,cr);
890 wallcycle_stop(wcycle,ewcVSITESPREAD);
894 if (flags & GMX_FORCE_VIRIAL)
896 /* Calculation of the virial must be done after vsites! */
897 calc_virial(fplog,mdatoms->start,mdatoms->homenr,x,f,
898 vir_force,graph,box,nrnb,fr,inputrec->ePBC);
902 enerd->term[F_COM_PULL] = 0;
903 if (inputrec->ePull == epullUMBRELLA || inputrec->ePull == epullCONST_F)
905 /* Calculate the center of mass forces, this requires communication,
906 * which is why pull_potential is called close to other communication.
907 * The virial contribution is calculated directly,
908 * which is why we call pull_potential after calc_virial.
910 set_pbc(&pbc,inputrec->ePBC,box);
911 dvdlambda[efptRESTRAINT] = 0;
912 enerd->term[F_COM_PULL] +=
913 pull_potential(inputrec->ePull,inputrec->pull,mdatoms,&pbc,
914 cr,t,lambda[efptRESTRAINT],x,f,vir_force,&(dvdlambda[efptRESTRAINT]));
917 fprintf(fplog,sepdvdlformat,"Com pull",enerd->term[F_COM_PULL],dvdlambda[efptRESTRAINT]);
919 enerd->dvdl_lin[efptRESTRAINT] += dvdlambda[efptRESTRAINT];
922 /* Add the forces from enforced rotation potentials (if any) */
925 wallcycle_start(wcycle,ewcROTadd);
926 enerd->term[F_COM_PULL] += add_rot_forces(inputrec->rot, f, cr,step,t);
927 wallcycle_stop(wcycle,ewcROTadd);
930 if (PAR(cr) && !(cr->duty & DUTY_PME))
932 cycles_ppdpme = wallcycle_stop(wcycle,ewcPPDURINGPME);
933 dd_cycles_add(cr->dd,cycles_ppdpme,ddCyclPPduringPME);
935 /* In case of node-splitting, the PP nodes receive the long-range
936 * forces, virial and energy from the PME nodes here.
938 wallcycle_start(wcycle,ewcPP_PMEWAITRECVF);
939 dvdlambda[efptCOUL] = 0;
940 gmx_pme_receive_f(cr,fr->f_novirsum,fr->vir_el_recip,&e,&dvdlambda[efptCOUL],
944 fprintf(fplog,sepdvdlformat,"PME mesh",e,dvdlambda[efptCOUL]);
946 enerd->term[F_COUL_RECIP] += e;
947 enerd->dvdl_lin[efptCOUL] += dvdlambda[efptCOUL];
950 dd_cycles_add(cr->dd,cycles_seppme,ddCyclPME);
952 wallcycle_stop(wcycle,ewcPP_PMEWAITRECVF);
955 if (bDoForces && fr->bF_NoVirSum)
959 /* Spread the mesh force on virtual sites to the other particles...
960 * This is parallellized. MPI communication is performed
961 * if the constructing atoms aren't local.
963 wallcycle_start(wcycle,ewcVSITESPREAD);
964 spread_vsite_f(fplog,vsite,x,fr->f_novirsum,NULL,
965 (flags & GMX_FORCE_VIRIAL),fr->vir_el_recip,
967 &top->idef,fr->ePBC,fr->bMolPBC,graph,box,cr);
968 wallcycle_stop(wcycle,ewcVSITESPREAD);
970 if (flags & GMX_FORCE_VIRIAL)
972 /* Now add the forces, this is local */
975 sum_forces(0,fr->f_novirsum_n,f,fr->f_novirsum);
979 sum_forces(start,start+homenr,f,fr->f_novirsum);
981 if (EEL_FULL(fr->eeltype))
983 /* Add the mesh contribution to the virial */
984 m_add(vir_force,fr->vir_el_recip,vir_force);
988 pr_rvecs(debug,0,"vir_force",vir_force,DIM);
993 /* Sum the potential energy terms from group contributions */
994 sum_epot(&(inputrec->opts),enerd);
996 if (fr->print_force >= 0 && bDoForces)
998 print_large_forces(stderr,mdatoms,cr,step,fr->print_force,x,f);
1002 void do_constrain_first(FILE *fplog,gmx_constr_t constr,
1003 t_inputrec *ir,t_mdatoms *md,
1004 t_state *state,rvec *f,
1005 t_graph *graph,t_commrec *cr,t_nrnb *nrnb,
1006 t_forcerec *fr, gmx_localtop_t *top, tensor shake_vir)
1009 gmx_large_int_t step;
1010 real dt=ir->delta_t;
1014 snew(savex,state->natoms);
1017 end = md->homenr + start;
1020 fprintf(debug,"vcm: start=%d, homenr=%d, end=%d\n",
1021 start,md->homenr,end);
1022 /* Do a first constrain to reset particles... */
1023 step = ir->init_step;
1026 char buf[STEPSTRSIZE];
1027 fprintf(fplog,"\nConstraining the starting coordinates (step %s)\n",
1028 gmx_step_str(step,buf));
1032 /* constrain the current position */
1033 constrain(NULL,TRUE,FALSE,constr,&(top->idef),
1034 ir,NULL,cr,step,0,md,
1035 state->x,state->x,NULL,
1036 state->box,state->lambda[efptBONDED],&dvdl_dum,
1037 NULL,NULL,nrnb,econqCoord,ir->epc==epcMTTK,state->veta,state->veta);
1040 /* constrain the inital velocity, and save it */
1041 /* also may be useful if we need the ekin from the halfstep for velocity verlet */
1042 /* might not yet treat veta correctly */
1043 constrain(NULL,TRUE,FALSE,constr,&(top->idef),
1044 ir,NULL,cr,step,0,md,
1045 state->x,state->v,state->v,
1046 state->box,state->lambda[efptBONDED],&dvdl_dum,
1047 NULL,NULL,nrnb,econqVeloc,ir->epc==epcMTTK,state->veta,state->veta);
1049 /* constrain the inital velocities at t-dt/2 */
1050 if (EI_STATE_VELOCITY(ir->eI) && ir->eI!=eiVV)
1052 for(i=start; (i<end); i++)
1054 for(m=0; (m<DIM); m++)
1056 /* Reverse the velocity */
1057 state->v[i][m] = -state->v[i][m];
1058 /* Store the position at t-dt in buf */
1059 savex[i][m] = state->x[i][m] + dt*state->v[i][m];
1062 /* Shake the positions at t=-dt with the positions at t=0
1063 * as reference coordinates.
1067 char buf[STEPSTRSIZE];
1068 fprintf(fplog,"\nConstraining the coordinates at t0-dt (step %s)\n",
1069 gmx_step_str(step,buf));
1072 constrain(NULL,TRUE,FALSE,constr,&(top->idef),
1073 ir,NULL,cr,step,-1,md,
1074 state->x,savex,NULL,
1075 state->box,state->lambda[efptBONDED],&dvdl_dum,
1076 state->v,NULL,nrnb,econqCoord,ir->epc==epcMTTK,state->veta,state->veta);
1078 for(i=start; i<end; i++) {
1079 for(m=0; m<DIM; m++) {
1080 /* Re-reverse the velocities */
1081 state->v[i][m] = -state->v[i][m];
1088 void calc_enervirdiff(FILE *fplog,int eDispCorr,t_forcerec *fr)
1090 double eners[2],virs[2],enersum,virsum,y0,f,g,h;
1091 double r0,r1,r,rc3,rc9,ea,eb,ec,pa,pb,pc,pd;
1092 double invscale,invscale2,invscale3;
1093 int ri0,ri1,ri,i,offstart,offset;
1096 fr->enershiftsix = 0;
1097 fr->enershifttwelve = 0;
1098 fr->enerdiffsix = 0;
1099 fr->enerdifftwelve = 0;
1101 fr->virdifftwelve = 0;
1103 if (eDispCorr != edispcNO) {
1104 for(i=0; i<2; i++) {
1108 if ((fr->vdwtype == evdwSWITCH) || (fr->vdwtype == evdwSHIFT)) {
1109 if (fr->rvdw_switch == 0)
1111 "With dispersion correction rvdw-switch can not be zero "
1112 "for vdw-type = %s",evdw_names[fr->vdwtype]);
1114 scale = fr->nblists[0].tab.scale;
1115 vdwtab = fr->nblists[0].vdwtab;
1117 /* Round the cut-offs to exact table values for precision */
1118 ri0 = floor(fr->rvdw_switch*scale);
1119 ri1 = ceil(fr->rvdw*scale);
1125 if (fr->vdwtype == evdwSHIFT) {
1126 /* Determine the constant energy shift below rvdw_switch */
1127 fr->enershiftsix = (real)(-1.0/(rc3*rc3)) - vdwtab[8*ri0];
1128 fr->enershifttwelve = (real)( 1.0/(rc9*rc3)) - vdwtab[8*ri0 + 4];
1130 /* Add the constant part from 0 to rvdw_switch.
1131 * This integration from 0 to rvdw_switch overcounts the number
1132 * of interactions by 1, as it also counts the self interaction.
1133 * We will correct for this later.
1135 eners[0] += 4.0*M_PI*fr->enershiftsix*rc3/3.0;
1136 eners[1] += 4.0*M_PI*fr->enershifttwelve*rc3/3.0;
1138 invscale = 1.0/(scale);
1139 invscale2 = invscale*invscale;
1140 invscale3 = invscale*invscale2;
1142 /* following summation derived from cubic spline definition,
1143 Numerical Recipies in C, second edition, p. 113-116. Exact
1144 for the cubic spline. We first calculate the negative of
1145 the energy from rvdw to rvdw_switch, assuming that g(r)=1,
1146 and then add the more standard, abrupt cutoff correction to
1147 that result, yielding the long-range correction for a
1148 switched function. We perform both the pressure and energy
1149 loops at the same time for simplicity, as the computational
1153 enersum = 0.0; virsum = 0.0;
1158 for (ri=ri0; ri<ri1; ri++) {
1161 eb = 2.0*invscale2*r;
1165 pb = 3.0*invscale2*r;
1166 pc = 3.0*invscale*r*r;
1169 /* this "8" is from the packing in the vdwtab array - perhaps
1170 should be #define'ed? */
1171 offset = 8*ri + offstart;
1172 y0 = vdwtab[offset];
1173 f = vdwtab[offset+1];
1174 g = vdwtab[offset+2];
1175 h = vdwtab[offset+3];
1177 enersum += y0*(ea/3 + eb/2 + ec) + f*(ea/4 + eb/3 + ec/2)+
1178 g*(ea/5 + eb/4 + ec/3) + h*(ea/6 + eb/5 + ec/4);
1179 virsum += f*(pa/4 + pb/3 + pc/2 + pd) +
1180 2*g*(pa/5 + pb/4 + pc/3 + pd/2) + 3*h*(pa/6 + pb/5 + pc/4 + pd/3);
1183 enersum *= 4.0*M_PI;
1185 eners[i] -= enersum;
1189 /* now add the correction for rvdw_switch to infinity */
1190 eners[0] += -4.0*M_PI/(3.0*rc3);
1191 eners[1] += 4.0*M_PI/(9.0*rc9);
1192 virs[0] += 8.0*M_PI/rc3;
1193 virs[1] += -16.0*M_PI/(3.0*rc9);
1195 else if ((fr->vdwtype == evdwCUT) || (fr->vdwtype == evdwUSER)) {
1196 if (fr->vdwtype == evdwUSER && fplog)
1198 "WARNING: using dispersion correction with user tables\n");
1199 rc3 = fr->rvdw*fr->rvdw*fr->rvdw;
1201 eners[0] += -4.0*M_PI/(3.0*rc3);
1202 eners[1] += 4.0*M_PI/(9.0*rc9);
1203 virs[0] += 8.0*M_PI/rc3;
1204 virs[1] += -16.0*M_PI/(3.0*rc9);
1207 "Dispersion correction is not implemented for vdw-type = %s",
1208 evdw_names[fr->vdwtype]);
1210 fr->enerdiffsix = eners[0];
1211 fr->enerdifftwelve = eners[1];
1212 /* The 0.5 is due to the Gromacs definition of the virial */
1213 fr->virdiffsix = 0.5*virs[0];
1214 fr->virdifftwelve = 0.5*virs[1];
1218 void calc_dispcorr(FILE *fplog,t_inputrec *ir,t_forcerec *fr,
1219 gmx_large_int_t step,int natoms,
1220 matrix box,real lambda,tensor pres,tensor virial,
1221 real *prescorr, real *enercorr, real *dvdlcorr)
1223 gmx_bool bCorrAll,bCorrPres;
1224 real dvdlambda,invvol,dens,ninter,avcsix,avctwelve,enerdiff,svir=0,spres=0;
1234 if (ir->eDispCorr != edispcNO) {
1235 bCorrAll = (ir->eDispCorr == edispcAllEner ||
1236 ir->eDispCorr == edispcAllEnerPres);
1237 bCorrPres = (ir->eDispCorr == edispcEnerPres ||
1238 ir->eDispCorr == edispcAllEnerPres);
1240 invvol = 1/det(box);
1243 /* Only correct for the interactions with the inserted molecule */
1244 dens = (natoms - fr->n_tpi)*invvol;
1249 dens = natoms*invvol;
1250 ninter = 0.5*natoms;
1253 if (ir->efep == efepNO)
1255 avcsix = fr->avcsix[0];
1256 avctwelve = fr->avctwelve[0];
1260 avcsix = (1 - lambda)*fr->avcsix[0] + lambda*fr->avcsix[1];
1261 avctwelve = (1 - lambda)*fr->avctwelve[0] + lambda*fr->avctwelve[1];
1264 enerdiff = ninter*(dens*fr->enerdiffsix - fr->enershiftsix);
1265 *enercorr += avcsix*enerdiff;
1267 if (ir->efep != efepNO)
1269 dvdlambda += (fr->avcsix[1] - fr->avcsix[0])*enerdiff;
1273 enerdiff = ninter*(dens*fr->enerdifftwelve - fr->enershifttwelve);
1274 *enercorr += avctwelve*enerdiff;
1275 if (fr->efep != efepNO)
1277 dvdlambda += (fr->avctwelve[1] - fr->avctwelve[0])*enerdiff;
1283 svir = ninter*dens*avcsix*fr->virdiffsix/3.0;
1284 if (ir->eDispCorr == edispcAllEnerPres)
1286 svir += ninter*dens*avctwelve*fr->virdifftwelve/3.0;
1288 /* The factor 2 is because of the Gromacs virial definition */
1289 spres = -2.0*invvol*svir*PRESFAC;
1291 for(m=0; m<DIM; m++) {
1292 virial[m][m] += svir;
1293 pres[m][m] += spres;
1298 /* Can't currently control when it prints, for now, just print when degugging */
1302 fprintf(debug,"Long Range LJ corr.: <C6> %10.4e, <C12> %10.4e\n",
1308 "Long Range LJ corr.: Epot %10g, Pres: %10g, Vir: %10g\n",
1309 *enercorr,spres,svir);
1313 fprintf(debug,"Long Range LJ corr.: Epot %10g\n",*enercorr);
1317 if (fr->bSepDVDL && do_per_step(step,ir->nstlog))
1319 fprintf(fplog,sepdvdlformat,"Dispersion correction",
1320 *enercorr,dvdlambda);
1322 if (fr->efep != efepNO)
1324 *dvdlcorr += dvdlambda;
1329 void do_pbc_first(FILE *fplog,matrix box,t_forcerec *fr,
1330 t_graph *graph,rvec x[])
1333 fprintf(fplog,"Removing pbc first time\n");
1334 calc_shifts(box,fr->shift_vec);
1336 mk_mshift(fplog,graph,fr->ePBC,box,x);
1338 p_graph(debug,"do_pbc_first 1",graph);
1339 shift_self(graph,box,x);
1340 /* By doing an extra mk_mshift the molecules that are broken
1341 * because they were e.g. imported from another software
1342 * will be made whole again. Such are the healing powers
1345 mk_mshift(fplog,graph,fr->ePBC,box,x);
1347 p_graph(debug,"do_pbc_first 2",graph);
1350 fprintf(fplog,"Done rmpbc\n");
1353 static void low_do_pbc_mtop(FILE *fplog,int ePBC,matrix box,
1354 gmx_mtop_t *mtop,rvec x[],
1359 gmx_molblock_t *molb;
1361 if (bFirst && fplog)
1362 fprintf(fplog,"Removing pbc first time\n");
1366 for(mb=0; mb<mtop->nmolblock; mb++) {
1367 molb = &mtop->molblock[mb];
1368 if (molb->natoms_mol == 1 ||
1369 (!bFirst && mtop->moltype[molb->type].cgs.nr == 1)) {
1370 /* Just one atom or charge group in the molecule, no PBC required */
1371 as += molb->nmol*molb->natoms_mol;
1373 /* Pass NULL iso fplog to avoid graph prints for each molecule type */
1374 mk_graph_ilist(NULL,mtop->moltype[molb->type].ilist,
1375 0,molb->natoms_mol,FALSE,FALSE,graph);
1377 for(mol=0; mol<molb->nmol; mol++) {
1378 mk_mshift(fplog,graph,ePBC,box,x+as);
1380 shift_self(graph,box,x+as);
1381 /* The molecule is whole now.
1382 * We don't need the second mk_mshift call as in do_pbc_first,
1383 * since we no longer need this graph.
1386 as += molb->natoms_mol;
1394 void do_pbc_first_mtop(FILE *fplog,int ePBC,matrix box,
1395 gmx_mtop_t *mtop,rvec x[])
1397 low_do_pbc_mtop(fplog,ePBC,box,mtop,x,TRUE);
1400 void do_pbc_mtop(FILE *fplog,int ePBC,matrix box,
1401 gmx_mtop_t *mtop,rvec x[])
1403 low_do_pbc_mtop(fplog,ePBC,box,mtop,x,FALSE);
1406 void finish_run(FILE *fplog,t_commrec *cr,const char *confout,
1407 t_inputrec *inputrec,
1408 t_nrnb nrnb[],gmx_wallcycle_t wcycle,
1409 gmx_runtime_t *runtime,
1410 gmx_bool bWriteStat)
1413 t_nrnb *nrnb_tot=NULL;
1416 double cycles[ewcNR];
1418 wallcycle_sum(cr,wcycle,cycles);
1420 if (cr->nnodes > 1) {
1424 MPI_Reduce(nrnb->n,nrnb_tot->n,eNRNB,MPI_DOUBLE,MPI_SUM,
1425 MASTERRANK(cr),cr->mpi_comm_mysim);
1431 if (SIMMASTER(cr)) {
1432 print_flop(fplog,nrnb_tot,&nbfs,&mflop);
1433 if (cr->nnodes > 1) {
1438 if ((cr->duty & DUTY_PP) && DOMAINDECOMP(cr)) {
1439 print_dd_statistics(cr,inputrec,fplog);
1451 snew(nrnb_all,cr->nnodes);
1452 nrnb_all[0] = *nrnb;
1453 for(s=1; s<cr->nnodes; s++)
1455 MPI_Recv(nrnb_all[s].n,eNRNB,MPI_DOUBLE,s,0,
1456 cr->mpi_comm_mysim,&stat);
1458 pr_load(fplog,cr,nrnb_all);
1463 MPI_Send(nrnb->n,eNRNB,MPI_DOUBLE,MASTERRANK(cr),0,
1464 cr->mpi_comm_mysim);
1469 if (SIMMASTER(cr)) {
1470 wallcycle_print(fplog,cr->nnodes,cr->npmenodes,runtime->realtime,
1473 if (EI_DYNAMICS(inputrec->eI)) {
1474 delta_t = inputrec->delta_t;
1480 print_perf(fplog,runtime->proctime,runtime->realtime,
1481 cr->nnodes-cr->npmenodes,
1482 runtime->nsteps_done,delta_t,nbfs,mflop);
1485 print_perf(stderr,runtime->proctime,runtime->realtime,
1486 cr->nnodes-cr->npmenodes,
1487 runtime->nsteps_done,delta_t,nbfs,mflop);
1491 runtime=inputrec->nsteps*inputrec->delta_t;
1493 if (cr->nnodes == 1)
1494 fprintf(stderr,"\n\n");
1495 print_perf(stderr,nodetime,realtime,runtime,&ntot,
1496 cr->nnodes-cr->npmenodes,FALSE);
1498 wallcycle_print(fplog,cr->nnodes,cr->npmenodes,realtime,wcycle,cycles);
1499 print_perf(fplog,nodetime,realtime,runtime,&ntot,cr->nnodes-cr->npmenodes,
1502 pr_load(fplog,cr,nrnb_all);
1509 extern void initialize_lambdas(FILE *fplog,t_inputrec *ir,int *fep_state,real *lambda,double *lam0)
1511 /* this function works, but could probably use a logic rewrite to keep all the different
1512 types of efep straight. */
1515 t_lambda *fep = ir->fepvals;
1517 if ((ir->efep==efepNO) && (ir->bSimTemp == FALSE)) {
1518 for (i=0;i<efptNR;i++) {
1527 *fep_state = fep->init_fep_state; /* this might overwrite the checkpoint
1528 if checkpoint is set -- a kludge is in for now
1530 for (i=0;i<efptNR;i++)
1532 /* overwrite lambda state with init_lambda for now for backwards compatibility */
1533 if (fep->init_lambda>=0) /* if it's -1, it was never initializd */
1535 lambda[i] = fep->init_lambda;
1537 lam0[i] = lambda[i];
1542 lambda[i] = fep->all_lambda[i][*fep_state];
1544 lam0[i] = lambda[i];
1549 /* need to rescale control temperatures to match current state */
1550 for (i=0;i<ir->opts.ngtc;i++) {
1551 if (ir->opts.ref_t[i] > 0) {
1552 ir->opts.ref_t[i] = ir->simtempvals->temperatures[*fep_state];
1558 /* Send to the log the information on the current lambdas */
1561 fprintf(fplog,"Initial vector of lambda components:[ ");
1562 for (i=0;i<efptNR;i++)
1564 fprintf(fplog,"%10.4f ",lambda[i]);
1566 fprintf(fplog,"]\n");
1572 void init_md(FILE *fplog,
1573 t_commrec *cr,t_inputrec *ir,const output_env_t oenv,
1574 double *t,double *t0,
1575 real *lambda, int *fep_state, double *lam0,
1576 t_nrnb *nrnb,gmx_mtop_t *mtop,
1578 int nfile,const t_filenm fnm[],
1579 gmx_mdoutf_t **outf,t_mdebin **mdebin,
1580 tensor force_vir,tensor shake_vir,rvec mu_tot,
1581 gmx_bool *bSimAnn,t_vcm **vcm, t_state *state, unsigned long Flags)
1586 /* Initial values */
1587 *t = *t0 = ir->init_t;
1590 for(i=0;i<ir->opts.ngtc;i++)
1592 /* set bSimAnn if any group is being annealed */
1593 if(ir->opts.annealing[i]!=eannNO)
1600 update_annealing_target_temp(&(ir->opts),ir->init_t);
1603 /* Initialize lambda variables */
1604 initialize_lambdas(fplog,ir,fep_state,lambda,lam0);
1608 *upd = init_update(fplog,ir);
1614 *vcm = init_vcm(fplog,&mtop->groups,ir);
1617 if (EI_DYNAMICS(ir->eI) && !(Flags & MD_APPENDFILES))
1619 if (ir->etc == etcBERENDSEN)
1621 please_cite(fplog,"Berendsen84a");
1623 if (ir->etc == etcVRESCALE)
1625 please_cite(fplog,"Bussi2007a");
1633 *outf = init_mdoutf(nfile,fnm,Flags,cr,ir,oenv);
1635 *mdebin = init_mdebin((Flags & MD_APPENDFILES) ? NULL : (*outf)->fp_ene,
1636 mtop,ir, (*outf)->fp_dhdl);
1641 please_cite(fplog,"Fritsch12");
1642 please_cite(fplog,"Junghans10");
1644 /* Initiate variables */
1645 clear_mat(force_vir);
1646 clear_mat(shake_vir);